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Cliff, L.

Publications and source records attributed to Cliff, L..

2 recordsLinked to original sources

Occupancy distributions of membrane proteins in heterogeneous liposome populations

Measurements of membrane protein structure and function often rely on reconstituting the protein into lipid bilayers through the formation of liposomes. Many measurements conducted in proteoliposomes, e.g. transport rates, single-molecule dynamics, monomer-oligomer equilibrium, require some understanding of the occupancy statistics of the liposome population for correct interpretation of the results. In homogenous liposomes, this is easy to calculate as the act of protein incorporation can be described by the Poisson distribution. However, in reality, liposomes are heterogeneous, which alters the statistics of occupancy in several ways. Here, we determine the liposome occupancy distribution for membrane protein reconstitution while taking into account liposome size heterogeneity. We calculate the protein occupancy for a homogenous population of liposomes with radius r = 200 nm, representing an idealization of vesicles extruded through 400 nm pores and compare it to the right-skewed distribution of 400 nm 2:1 POPE:POPG vesicles. As is the case for E. coli polar lipids, this synthetic composition yields a sub-population of small liposomes, [~]25 nm in radius with a long tail of larger vesicles. Previously published microscopy data of the co-localization of the CLC-ec1 Cl-/H+ transporter with liposomes, and vesicle occupancy measurements using functional transport assays, shows agreement with the heterogeneous 2:1 POPE:POPG population. Next, distributions of 100 nm and 30 nm extruded 2:1 POPE:POPG liposomes are measured by cryo-electron microscopy, demonstrating that extrusion through smaller pores does not shift the peak, but reduces polydispersity arising from large liposomes. Single-molecule photobleaching analysis of CLC-ec1-Cy5 shows the 30 nm extruded population increases the Poisson-dilution range, reducing the probability of vesicles with more than one protein at higher protein/lipid densities. These results demonstrate that the occupancy distributions of membrane proteins into vesicles can be accurately predicted in heterogeneous populations with experimental knowledge of the liposome size distribution.

biophysics↗

A model-free method for measuring dimerization free energies of CLC-ec1 in lipid bilayers

We previously reported the equilibrium dimerization reaction of the CLC-ec1 Cl-/H+ transporter in 2:1 POPE/POPG membranes (Chadda et al. 2016). This was determined by measuring the probability distributions of subunit capture into extruded liposomes by single-molecule photobleaching analysis across a wide range of subunit/lipid mole fraction densities. In this approach, knowledge of the liposome size distribution is necessary in order to correct the data for random co-capture events and extract the underlying dimerization reaction. For this we used a previously reported cryo-electron microscopy (cryo-EM) measured size distribution of 400 nm extruded liposomes made of E. coli polar lipids (Walden et al. 2007). While the model and data agreed at low densities, we observed systematic inaccuracies at higher densities limiting our ability to extract FDimer in this range. To address this issue, we measured the 400 nm extruded 2:1 POPE/POPG liposome size distribution by cryo-EM and found that there is a small, but significant amount of larger liposomes in the population. Re-analysis of the I201W/I422W WW photobleaching data using this distribution shows that the protein is monomeric in the membrane and can serve as an experimental control. Dimer controls were constructed by glutaraldehyde cross-linking of C85A/H234C WT or introducing R230C/L249C, which forms a spontaneous disulfide bond. Determination of FDimer based on the experimental controls yields improved fits and no change in the previously reported{Delta} G{degrees} values, providing an alternate model-free approach to measuring CLC-ec1 dimerization in membranes.

biochemistry↗